Find the increase in the length of the rod

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The discussion revolves around calculating the increase in length of a metal rod subjected to a non-uniform temperature distribution described by T(x) = T_0 sin(πx/L). The initial attempt incorrectly used a differential temperature change, leading to a result of zero. Clarification was provided that the correct approach involves using the finite temperature difference ΔT instead of dT. The final expression for the increase in length is derived as ΔL = (2LαT_0) / π, confirmed through integration of the temperature function. The conversation emphasizes the importance of accurately applying thermal expansion principles in the context of varying temperatures along the rod.
utkarshakash
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Homework Statement


A metal rod of length L at temperature of 0°C is not uniformly heated such that the temperature is given by the distance x along its length measured from one end when:
T(x) = T_0 \sin (\pi x/L)
Accordingly, points at x = 0 and x = L are also zero temperature, whereas at x = L/2, where the argument of sine function is π/2, the temperature have the maximum value T0. The coefficient of linear expansion of the rod is α. Find the increase in the length of the rod in function of α and T0.

The Attempt at a Solution



Let us consider a differential element dx at a distance x from one end of the rod.

Δ(dx) = dx \alpha dT \\<br /> ΔL = \alpha T_0 \displaystyle \int_0^L \cos \left( \dfrac{\pi x}{L} \right) dx

But the above equation gives me 0! :confused:
I know something's going wrong here.
 
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utkarshakash said:
Δ(dx) = dx \alpha dT<br />
Careful. That should be ΔT, not dT. The temperature difference is a finite function of x, not a differential. (And if it's with respect to 0°, then ΔT = T.)
 
Doc Al said:
Careful. That should be ΔT, not dT. The temperature difference is a finite function of x, not a differential. (And if it's with respect to 0°, then ΔT = T.)

Thanks!
 
What is the answer ?
 
2L \alpha T_0 / \pi
 
utkarshakash said:
2L \alpha T_0 / \pi

Could you please show how you got this answer.
 
Tanya Sharma said:
Could you please show how you got this answer.

Sure.

Let's consider a differential element dx at a distance x from one end of the rod.
Δ(dx) = dx \alpha (t(0) - t(x)) \\<br /> =- \alpha T_0 \sin \dfrac{\pi x}{L} dx \\<br />

Integrating both sides

ΔL = \dfrac{- L \alpha T_0}{\pi} \left( \cos \dfrac{\pi x}{L} \right)_0^L

Substitute the values to get the answer.
 
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utkarshakash said:
Sure.

Let's consider a differential element dx at a distance x from one end of the rod.
Δ(dx) = dx \alpha (t(0) - t(x)) \\<br /> =- \alpha T_0 \sin \dfrac{\pi x}{L} dx \\<br />

Integrating both sides

ΔL = \dfrac{- L \alpha T_0}{\pi} \left( \cos \dfrac{\pi x}{L} \right)_0^L

Substitute the values to get the answer.

Thanks a lot :)
 

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